Method and apparatus for the correction of magnetic resonance scan data

ABSTRACT

In a method and magnetic resonance (MR) apparatus for correcting MR scan data, an MR scanner is operated to acquire first and second correction data sets respectively from first and second sub-volumes of a correction volume, by successive executions of an echo planar imaging sequence. The MR scanner is also operated to acquire third and fourth correction data sets respectively from third and fourth correction sub-volumes, also by successive executions of the echo planar imaging sequence. A first item of correction information is ascertained from the first and second correction data sets, and a second item of correction information is ascertained from the third and fourth correction data sets. The first and second items of correction information are then used to correct scan data, also acquired with the MR scanner.

BACKGROUND OF THE INVENTION Field of the Invention

The invention concerns a method for the correction of magnetic resonancescan data, and a magnetic resonance device and a non-transitory datastorage medium that implement such a method.

Description of the Prior Art

In a magnetic resonance (MR) apparatus, also called a magnetic resonancetomography system, the body of an examination person, in particular apatient, to be examined is placed in an MR data acquisition scanner andconventionally exposed therein to a relatively high basic magneticfield, for example of 1.5 or 3 or 7 tesla, produced by a basic fieldmagnet of the scanner. In addition, gradient switchings are activated bythe operation of gradient coils. Radio-frequency pulses, for exampleexcitation pulses, are then emitted by a radio-frequency antenna unit bysuitable antenna devices, and this leads to the nuclear spins ofspecific atoms, excited in a resonant manner by these radio-frequencypulses being tilted by a defined flip angle with respect to the magneticfield lines of the basic magnetic field. As the nuclear spins relax,radio-frequency signals, what are known as magnetic resonance signals,are emitted therefrom, which are received by suitable radio-frequencyantennae and then processed further. Finally, the desired image data canbe reconstructed from the raw data acquired in this way.

For a specific scan, a specific magnetic resonance sequence, also calleda pulse sequence, should be emitted, which is composed of a sequence ofradio-frequency pulses, for example excitation pulses and refocusingpulses, and appropriate gradient switching operations that are to beemitted in a coordinated manner in various gradient axes in variousdirections. At a time appropriate therewith, readout windows are set,and these specify the periods in which the induced magnetic resonancesignals are detected.

A known method for magnetic resonance imaging is an echo planar imagingmethod, which is also called echo planar imaging (EPI). The echo planarimaging method is implemented using an echo planar imaging magneticresonance sequence (EPI sequence). In an EPI sequence of this kind,multiple phase-coded echoes are successively generated by gradientrefocusing in order to fill a raw data matrix in a memory, calledk-space. A sequence of echoes of this kind is also called an EPI echotrain. The EPI echo train is typically recorded following a single,possibly selective, radio-frequency excitation. Iteration of a row of ak-space to be recorded is typically carried out between the echoes bygradient switching operations in the phase coding direction.

The PLACE imaging method is known from the article by Xiang and Ye,“Correction for Geometric Distortion and N/2 Ghosting in EPI by PhaseLabeling for Additional Coordinate Encoding (PLACE)”, Magnetic Resonancein Medicine 57:731-741 (2007), PLACE stands for phase labeling foradditional coordinate encoding. The PLACE imaging method allows fastacquisition of a shift map and/or a B0 field map using magneticresonance image data, known as correction data sets, acquired byexecution of an echo planar imaging method. In the PLACE imaging method,data from a correction volume are acquired twice, in rare cases eventhree or four times, wherein the second acquisition is phase shiftedwith respect to the first acquisition, in particular in a phase codingdirection. The shift map and/or B0 field map can be calculated from thecorrection data sets acquired in the first and second acquisitions, asdescribed in detail in the document by Xiang and Ye. The shift mapand/or B0 field map can then be used for correction of magneticresonance scan data. In this connection the shift map and/or the B0field map can be used, in particular, for correction of inhomogeneitiesin a main magnetic field of the magnetic resonance device. Originalpositions, for example, of distorted and/or shifted image points inmagnetic resonance scan data, can be restored using the shift map.

In typical applications an examination volume for magnetic resonanceimaging, and therewith also a correction volume of the PLACE imagingmethod, is composed of multiple parallel slices which form a slicestack. In the conventional PLACE imaging method, first the entirecorrection volume, i.e. the entire slice stack, is completely acquiredin the first acquisition and then the entire correction volume iscompletely acquired again in the second acquisition. In the conventionalPLACE imaging method there is accordingly a time difference from arepetition time, which is required for the acquisition of the entirecorrection volume, between the two repetitions of the acquisition of thesame slice of the correction volume.

SUMMARY OF THE INVENTION

An object of the invention is to enable improved correction of magneticresonance scan data.

The inventive method for magnetic resonance imaging of an examinationobject by operation of a magnetic resonance scanner includes thefollowing method steps.

A first correction data set is acquired by execution of an echo planarimaging (data acquisition sequence) method from a first correctionsub-volume of a correction volume.

A second correction data set is acquired from the first correctionsub-volume, by another execution of the echo planar imaging method (dataacquisition sequence), with the second correction data set beingacquired phase shifted in relation to the first correction data set, andthe first correction data set and second correction data set beingacquired one immediately after the other.

A first item of correction information is ascertained in a computer fromthe first correction data set and the second correction data set.

A third correction data set is acquired from a second correctionsub-volume of the correction volume, by another execution of the echoplanar imaging method (data acquisition sequence).

A fourth correction data set is acquired from the second correctionsub-volume by another execution of the echo planar imaging method (dataacquisition sequence), with the fourth correction data set beingacquired phase shifted in relation to the third correction data set, andthe third correction data set and fourth correction data set beingacquired one immediately after the other.

A second item of correction information is ascertained in the computerfrom the third correction data set and the fourth correction data set.

A magnetic resonance scan data set is acquired from an examinationvolume.

The magnetic resonance scan data are corrected in the computer using thefirst item of correction information and second item of correctioninformation.

The examination object can be a patient, a training person, an animal ora phantom. The examination volume, also called the field of view (FOV),can be a volume that is mapped (represented) in the recorded magneticresonance image data. The examination volume is typically set by a user,for example on a localizer. Of course the examination volume canalternatively or additionally also be set automatically, for example onthe basis of a chosen protocol.

The correction volume can correspond to the examination volume. Thecorrection volume can also be designed to be different spatially fromthe examination volume, for example greater or smaller than theexamination volume and/or be spatially shifted and/or rotated withrespect to the examination volume. It can then be advantageous tointerpolate the correction information spatially from the correctionvolume on the examination volume. The entire correction volume includesthe first correction sub-volume and the second correction sub-volume.The first correction sub-volume can be designed to be spatially disjunctfrom the second correction sub-volume.

The first correction sub-volume and the second correction sub-volumetogether can form the correction volume. In addition to the firstcorrection sub-volume and the second correction sub-volume, thecorrection volume can alternatively also include at least one furthercorrection sub-volume that is spatially disjunct from the firstcorrection sub-volume and second correction sub-volume. Furthercorrection data sets are then acquired from the at least one furthercorrection sub-volume from the further correction data sets. Acquisitionof the further correction data sets can occur analogously to acquisitionof the first and second correction data sets or the third and fourthcorrection data sets solely from a different correction sub-volume ofthe correction volume. At least one further item of correctioninformation can then be ascertained from the further correction datasets, and the magnetic resonance scan data can then be corrected alsousing the at least one further item of correction information.

The magnetic resonance scan data can be raw data that are typically notdirectly available to an expert for the purpose of diagnosis. Themagnetic resonance scan data can also be magnetic resonance image datawhich can be displayed on a display unit and/or made available to anexpert in order to make a diagnosis. The magnetic resonance scan datacan also partly include the first, second, third and fourth correctiondata sets and/or be reconstructed from the first, second, third andfourth correction data sets. Of course it is also conceivable for thefirst, second, third and fourth correction data sets to be acquired inaddition to the magnetic resonance scan data.

The first item of correction information can be ascertained from thefirst and second correction data sets and the second item of correctioninformation can be ascertained from the third and fourth correction datasets using a method known to those skilled in the art, for example asdescribed in the aforementioned article by Xiang and Ye. The correctionof the magnetic resonance scan data using the first correctioninformation and the second correction information can be a correction ofa first part of the magnetic resonance scan data using the firstcorrection information and a correction of a second part of the magneticresonance scan data using the second correction information. The firstpart of the magnetic resonance scan data can be acquired from a firstsub-volume of the examination volume, which corresponds to the firstcorrection sub-volume, while the second part of the magnetic resonancescan data can be acquired from a second sub-volume of the examinationvolume, which corresponds to the second correction sub-volume.

The magnetic resonance scan data can be corrected using the first itemof correction information and the second item of correction informationby a method known to those skilled in the art. The first correctioninformation and the second correction information can be, for example,parts of a B0 field map and/or pixel shift map, using which the magneticresonance scan data are corrected. In this context the first correctioninformation and the second correction information can also be used forthe correction of artifacts in the magnetic resonance scan data, suchas, in the aforementioned article by Xiang and Ye. For example,geometric distortions and/or ghosting artifacts, which occur in thephase coding direction as a consequence of undesirable signalmodulations during EPI recordings that last a relatively long time, canbe corrected by using the first item of correction information and thesecond item of correction information. The corrected magnetic resonancescan data and/or magnetic resonance image data reconstructed from thecorrected magnetic resonance scan data can then be emitted as an outputdata file, for display to a user on a display monitor, and/or forstorage in a database.

The acquisition of the first correction data set and the secondcorrection data set so as to be phase shifted in relation to each othermeans that the first correction data set and the second correction dataset are entered into k-space along respective trajectories that areshifted in relation to each other by a phase shift in the phase codingdirection (which defines one axis of k-space). The first correction dataset and the second correction data set can have a phase shift of onephase blip or two phase blips or three phase blips. A phase blip is ashift in the phase coding direction that is caused by a small gradientpulse of the phase coding gradient of the EPI sequence. The shift in thephase coding direction can also be achieved by the use of different echotimes when acquiring the first correction data set and second correctiondata set. Of course a larger phase shift between the first correctiondata set and the second correction data set can also exist. The k spacerespective trajectories, which are used for acquiring the firstcorrection data set and the second correction data set, are shifted byone or more line(s) in the phase coding direction in this way. The sameapplies to the acquisition of the third correction data set and fourthcorrection data set in a manner phase-shifted in relation to each other.There is a first phase shift between the first correction data set andthe second correction data set, and a second phase shift between thethird correction data set and the fourth correction data set, with thefirst phase shift being equal to the second phase shift.

Acquisition of the first, second, third and fourth correction data setsis implemented by the operation of a magnetic resonance scanner. Thatthe first correction data set and second correction data set areacquired immediately, in succession, for example by acquisition of thesecond correction data set beginning as soon as acquisition of the firstcorrection data set is finished. In this way acquisition of the secondcorrection data set advantageously directly follows acquisition of thefirst correction data set. An interval between the start times ofacquisition of the first correction data set and of the secondcorrection data set can in this way be less than 250 ms, advantageouslyless than 150 ms, particularly advantageously less than 100 ms, and mostadvantageously less than 50 ms. No other scan data is acquired betweenacquisition of the first correction data set and of the secondcorrection data set. The third correction data set and the fourthcorrection data set can be acquired one immediately after the other inthe same way as just described.

In contrast to the conventional PLACE imaging method, in which first theentire correction volume is acquired and is then repeatedly acquiredagain in a phase-shifted manner, the inventive process providesacquisition of the correction volume in sections of each of two scans,which are phase shifted in relation to each other. In this way,according to the invention, first the first correction sub-volume isacquired in a phase shifted manner in two immediately successiverepetitions and later the second correction sub-volume is acquired in aphase shifted manner in two immediately successive repetitions. In otherwords, phase-shifted repetitions of acquisition of parts of thecorrection volume should occur even before acquisition of the entirecorrection volume is complete. The procedure is preferably performedslice-by-slice, as described in more detail below.

This procedure enables good correction of the magnetic resonance scandata, because the interval between repeated acquisition of thecorrection sub-volumes can be significantly reduced compared to theconventional PLACE imaging method. In this way it can be ensured thatthe correction data sets from which the correction information isascertained, for example the first correction data set and the secondcorrection data set, can be acquired consistently in relation to eachother. In this way the effect of a movement, such as a respiratorymovement and/or a cardiac movement and/or a movement of limbs, of theexamination object on the repeated acquisition of the correction datasets can be reduced. For example, a change in a lung position or achange in an oxygen concentration between different respiratory statescan exert an effect on the phase of acquired magnetic resonance scandata in a lung region of the examination object and/or in a region ofthe body of the examination object positioned at a distance from thelung region. The first correction data set and the second correctiondata set in accordance with the invention are therefore acquired in thesame respiratory state of the examination object. The quality of thefirst item of correction information and the second item of correctioninformation thus can be increased, because this is less adverselyaffected by movement of the examination object. With the inventiveprocedure the sensitivity of the correction of the magnetic resonancescan data to movement of the examination object can be reduced in thisway.

In an embodiment, the first correction sub-volume constitutes a firstpartial slice stack of the correction volume that has, at most, tenfirst slices of the correction volume that has, and the secondcorrection sub-volume constitutes a second partial slice stack of thecorrection volume that has, at most, ten second slices of the correctionvolume. The first correction sub-volume or the second correctionsub-volume preferably are only a portion of the slices of the correctionvolume, namely, at most, 50 percent of the slices of the correctionvolume, more preferably at most 30 percent of the slices of thecorrection volume, more preferably at most 15 percent of the slices ofthe correction volume, and most preferably at most 5 percent of theslices of the correction volume. The first partial slice stack of thecorrection volume has at most six, preferably at most four, morepreferably at most three, and most preferably at most two first slicesof the correction volume. The second partial slice stack of thecorrection volume has at most six, preferably at most four, morepreferably at most three, and most advantageously at most two secondslices of the correction volume. The reduction in the number of slicesof the correction sub-volume makes it possible to further reduce aninterval between the repeated acquisition of the correction sub-volumes.In this way, the sensitivity of ascertainment of the first and seconditems of correction information to movements of the examination objectcan be reduced further.

In another embodiment, the first correction sub-volume is a single firstslice of the correction volume and the second correction sub-volumeconstitutes a single second slice of the correction volume. In this waytwo correction data sets that are phase shifted in relation to eachother are acquired one immediately after the other, in particular forthe same slice respectively, from which sets an item of correctioninformation is then ascertained. For example, the first correction dataset is acquired from a specific slice of the correction volume anddirectly thereafter the second correction data set is acquired from thesame slice of the correction volume in a manner phase shifted inrelation to first correction data set. The third and fourth correctiondata sets can be analogously acquired one immediately after the otherfrom the same slice. This same slice being different from the slice ofthe correction volume from which the first and second correction datasets are acquired. In other words, the two correction data sets shouldbe acquired for a single slice, one immediately after the other, beforefurther correction data sets are acquired for a further slice. Becausethe correction sub-volumes have only one slice, the interval between therepeated acquisition of the correction sub-volumes can be particularlyadvantageously shortened. In this way, the sensitivity of ascertainmentof the first and second items of correction information to movements ofthe examination object can be particularly advantageously reduced.

In another embodiment, when acquiring the first correction data, a firstradio-frequency excitation pulse is used, when acquiring the secondcorrection data set a second radio-frequency excitation pulse is used,when acquiring the third correction data set a third radio-frequencyexcitation pulse is used and when acquiring the fourth correction dataset a fourth radio-frequency excitation pulse is used. The excitationpulses are used to excite the spins so the magnetic resonance signalsfor creating the correction data sets can be acquired. The magneticresonance signals, from which the first, second, third and fourthcorrection data sets are created, are each acquired in different readouttrains. A different excitation pulse should precede the differentreadout trains according to this embodiment. In this way, fourexcitation pulses thus are used to acquire the four correction data setstherefore. The use of separate excitation pulses to acquire the first,second, third and fourth correction data sets has the advantage that aspin ensemble for acquiring the magnetic resonance signals, from whichthe first, second, third and fourth correction data sets are created, isexcited once again in each case. When reading out the magnetic resonancesignals, from which the first, second, third and fourth correction datasets are created, the spins therefore advantageously each have the sameexcitation state. In this way the same conditions, for example the samegeometric distortions, exist when acquiring the first, second, third andfourth correction data sets. This achieves accurate consistency in thescan conditions, particularly during acquisition of the first and secondcorrection data sets, or during acquisition of the third and fourthcorrection data sets. The quality of the first item of correctioninformation and second item of correction information thus can beimproved further.

The excitation pulses of the radio-frequency excitation pulse set cantypically have a flip angle of 90°. As described in the followingparagraph, smaller flip angles can also be used for the excitationpulses. In particular applications it can be advantageous for the secondradio-frequency excitation pulse and the fourth radio-frequencyexcitation pulse to be configured as refocusing pulses. The secondradio-frequency excitation pulse and the fourth radio-frequencyexcitation pulse then have a flip angle of more than 90°, advantageously180°. In this way a magnetization excited by the first radio-frequencyexcitation pulse and the third radio-frequency excitation pulse can alsobe used when acquiring the second correction data set and the fourthcorrection data set.

In another embodiment, at least one radio-frequency excitation pulsefrom a radio-frequency excitation pulse set, which includes the firstradio-frequency excitation pulse, the second radio-frequency excitationpulse, the third radio-frequency excitation pulse and the fourthradio-frequency excitation pulse, has a flip angle of less than 50°. Inparticular, each radio-frequency excitation pulse of the radio-frequencyexcitation pulse set has a flip angle of less than 50°. The at least oneradio-frequency excitation pulse, in particular each radio-frequencyexcitation pulse of radio-frequency excitation pulse set, has a flipangle of less than 30°, preferably of less than 15°, more preferably ofless than 10°, and most preferably of less than 5°. This procedure isbased on the consideration that when creating the first item ofcorrection information from the first and second correction data sets,or when creating the second item of correction information from thethird and fourth correction data sets, a lower signal-to-noise ratio inthe first and second correction data sets or the third and fourthcorrection data sets, which is caused by the use of smaller flip angles,is typically of no consequence. Instead, the first item of correctioninformation can be ascertained from the first and second correction datasets, or the second item of correction information from the third andfourth correction data sets using the different image phases in thefirst and second correction data sets or third and fourth correctiondata sets. This information is independent of the flip angle used whenacquiring the correction data sets. Radio-frequency excitation pulseswith different flip angles can also be used for acquiring the first andsecond correction data sets or the third and fourth correction data setssince different image contrasts are not typically a problem whencreating the first and second items of correction information. Areduction in the flip angle of the at least one radio-frequencyexcitation pulse has the advantage that the stationary state (steadystate) is affected to a particularly small extent by the at least oneradio-frequency excitation pulse.

In another embodiment, first radio-frequency excitation pulse and thesecond radio-frequency excitation pulse have different first phases fromeach other and the third radio-frequency excitation pulse and the fourthradio-frequency excitation pulse have different second phases from eachother. In this way a radio-frequency spoiling between acquisition of thefirst and second correction data sets or of the third and fourthcorrection data sets can be implemented. This avoids signal excitationsfrom the first correction data set affecting acquisition of the secondcorrection data set, or signal excitations from the third correctiondata set affecting acquisition of the fourth correction data set. Inthis way the same recording conditions can be ensured during acquisitionof the first and second correction data sets, and acquisition of thethird and fourth correction data sets, respectively.

In another embodiment, between acquisition of the first and secondcorrection data sets, a first spoiler gradient pulse is activated fordephasing a residual magnetism, and between acquisition of the thirdcorrection data set and fourth correction data set a second spoilergradient pulse is activated for dephasing a residual magnetism. Thefirst spoiler gradient pulse is activated following conclusion of theEPI readout train, which is carried out in order to acquire the magneticresonance signals for the first correction data set. The first spoilergradient pulse is activated before the second radio-frequency excitationpulse, which is activated in order to acquire the second correction dataset. The second spoiler gradient pulse is analogously activatedfollowing acquisition of the third correction data set and before thestart of acquisition of the fourth correction data set. The firstspoiler gradient pulse dephases a residual magnetism that is presentfollowing acquisition of the first correction data set. In the same waythe second spoiler gradient pulse dephases a residual magnetism that ispresent following acquisition of the third correction data set. In thisway the same recording conditions can be ensured during acquisition ofthe first and second correction data sets, and acquisition of the thirdand fourth correction data sets, respectively.

In another embodiment, the first correction data set, the secondcorrection data set, the third correction data set and the fourthcorrection data set are acquired before acquisition of the magneticresonance scan data. In this way the correction data sets can beacquired in a pre-scan before the actual acquisition of the magneticresonance scan data. The pre-scan can be implemented particularlyquickly. Acquisition of the first, second, third and fourth correctiondata sets thus can be complete before acquisition of the magneticresonance scan data.

In another embodiment, the acquisition of the magnetic resonance scandata includes a first scan of the examination volume, a second scan ofthe examination volume and a third scan of the examination volume,wherein the first correction data set and the second correction data setare acquired between the first scan and the second scan of theexamination volume and the third correction data set and the fourthcorrection data set are acquired between the second scan and the thirdscan of the examination volume. In this way the examination volume isacquired repeatedly, in at least three scans. Magnetic resonance scandata from the entire examination volume are acquired in the first scan,second scan and third scan. A time series scan of the examinationvolume, such as for a functional magnetic resonance examination, can becarried out in this way. The claimed procedure can of course also becarried out analogously for further scans of the examination volume. Themagnetic resonance scan data and the correction data sets can beadvantageously alternately acquired in this way. This can be expedient,for example, if the correction data sets are to be updated during theongoing scanning of the magnetic resonance scan data. Furthermore, anoverall scan time for recording the magnetic resonance scan data and thecorrection data sets can be reduced in this way. As one suitable optiona first partial slice stack, in particular a first single slice, of thecorrection volume can be repeatedly acquired between the first scan andthe second scan of the examination volume. A second partial slice stack,in particular a second single slice, of the correction volume can thenbe repeatedly acquired between the second scan and the third scan of theexamination volume. The first partial slice stack and the second partialslice stack can have different slices of the correction volume from eachother. The slices of the partial slice stack of the correction volume,which are acquired between the scans of the examination volume, can becyclically shifted in this way. During acquisition of the correctiondata sets, which is inserted between the scans of the examinationvolume, a matrix size of the correction data sets can be reduced tofurther reduce the scan time for acquisition of the correction datasets. An interpolation of the scan data of the correction data sets forascertaining the correction information can occur in the process.

In another embodiment, the first correction data set, the secondcorrection data set, the third correction data set and the fourthcorrection data set form at least part of the magnetic resonance scandata. Of course the correction data sets can also form all of themagnetic resonance scan data. The slices recorded during acquisition ofthe correction data sets can be combined in this way to form at leastpart of the examination volume. A cyclical shift of the slices duringacquisition of the correction data sets, which form the magneticresonance scan data at least in part, can occur if the examinationvolume, as described in the preceding paragraph, is to be repeatedlyrecorded. The correction data sets can fulfill an advantageous dual rolein this proposed procedure. First, the correction data sets can be atleast a part of the magnetic resonance scan data. Secondly, thecorrection data can be used for correction of the magnetic resonancescan data. In this way the scan time can be reduced further and/or aparticularly appropriate correction of the magnetic resonance scan datacan be achieved due to the consistency of the magnetic resonance scandata and the correction data sets used for correction of the magneticresonance scan data.

The inventive magnetic resonance apparatus has a scanner that isoperated to acquire the first correction data set, the second correctiondata set, the third correction data set, the fourth correction data set,and a scan data set and a computer configured to execute the inventivemethod as described above.

The magnetic resonance apparatus is designed for carrying out a methodfor magnetic resonance imaging an examination object. The MR dataacquisition scanner is operated to acquire a first correction data set,by execution of an echo planar imaging sequence, from a first correctionsub-volume of a correction volume. The MR data acquisition scanner isoperated to acquire a second correction data set, by execution of theecho planar imaging sequence, from the first correction sub-volume, withthe second correction data set being acquired phase shifted in relationto the first correction data set, and the first correction data set andthe second correction data set being acquired one immediately after theother. The computer (or a processor thereof) is configured to ascertaina first item of correction information from the first correction dataset and the second correction data set. The MR data acquisition scanneris operated to acquire a third correction data set, by execution of theecho planar imaging sequence, from a second correction sub-volume of thecorrection volume. The MR data acquisition scanner is operated toacquire a fourth correction data set, by execution of the echo planarimaging sequence, from the second correction sub-volume, with the fourthcorrection data set being acquired phase shifted in relation to thethird correction data set, and the third correction data set and thefourth correction data being acquired one immediately after the other.The computer (or a processor thereof) is configured to ascertain asecond item of correction information from the third correction data setand the fourth correction data set. The MR data acquisition scanner isoperated to acquire magnetic resonance scan data from an examinationvolume. The computer (or a processor thereof) is configured to correctthe magnetic resonance scan data using the first item of correctioninformation and the second item of correction information.

The ascertaining of the first and second items of correctioninformation, and the correction of the scan data, can take placerespectively in processors or other modules of the computer.Alternatively, the processors may be individual stand-alone processorsthat are connected via a bus or a network, or all of the processors maybe combined as a single overall processor within the computer.

The invention also encompasses a non-transitory, computer-readable datastorage medium that can be loaded directly into a memory of aprogrammable computer of a magnetic resonance computer and has programcode that cause the inventive method to be implemented when the code isexecuted in the computer of the magnetic resonance device. The inventivemethod can consequently be carried out quickly, robustly and in a mannerthat can be repeated identically. The computer must have, for example,an appropriate main memory, an appropriate graphics card or anappropriate logic unit, so the respective method steps can be carriedout efficiently.

Examples of electronically readable data carriers are a DVD, magnetictape or a USB stick, on which electronically readable code, inparticular software is stored.

The advantages of the inventive storage medium and of the inventivemagnetic resonance apparatus essentially correspond to the advantages ofthe inventive method, which have been described above in detail.Features, advantages or alternative embodiments mentioned in connectionwith the method are similarly applicable transferred to the otheraspects of the invention. The corresponding functional features of themethod are performed by appropriate modules, in particular by hardwaremodules.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 shows an inventive magnetic resonance apparatus in a blockdiagram.

FIG. 2 is a flowchart of a first embodiment of the inventive method.

FIG. 3 is a diagram of a sequence over time of a second embodiment of aninventive method.

FIG. 4 is a diagram of a sequence over time of a third embodiment of aninventive method.

FIG. 5 is a diagram of a sequence over time of a fourth embodiment of aninventive method.

FIG. 6 is a diagram of a sequence over time of a fifth embodiment of aninventive method.

FIG. 7 is shows a diagram of a sequence over time of a sixth embodimentof an inventive method.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

FIG. 1 schematically shows an inventive magnetic resonance apparatus 11.The magnetic resonance apparatus 11 has an MR data acquisition scanner13, having a basic magnet 17 that generates a strong and constant basicmagnetic field 18. The MR data acquisition scanner 13 has a cylindricalpatient-receiving region 14 for receiving an examination object 15, inthe present case a patient. The patient-receiving region 14 iscylindrically surrounded in a circumferential direction by the scanner13. The patient 15 can be moved by a patient-positioning device 16 ofthe magnetic resonance apparatus 11 into the patient-receiving region14. The patient-positioning device 16 has for this purpose anexamination table arranged so as to move inside the scanner 13. Thescanner 13 is shielded from the outside by a housing shell 31.

The scanner 13 also has a gradient coil arrangement 19 that is operatedto generate magnetic field gradients that are used for spatial encodingthe MR signals. The gradient coil arrangement 19 is controlled by agradient control processor 28. The scanner 13 also has a radio-frequencyantenna unit (RF radiator) 20, which is designed in the illustrated caseas a body coil permanently integrated in the scanner 13, and aradio-frequency antenna control processor 29. The radio-frequencyantenna unit 20 is controlled by the radio-frequency antenna controlprocessor 29 so as to radiate radio-frequency magnetic resonancesequences into an examination space, which is essentially formed by thepatient-receiving region 14. The radio-frequency energy radiated by theradio-frequency antenna unit 20 excites selected nuclear spins in thepatient 15 so as to cause the excited nuclear spins to deviate from thepolarization or alignment produced by the basic magnetic field 18. Asthe excited nuclear spins relax, they emit magnetic resonance signals.The radio-frequency antenna unit 20 is also designed to receive magneticresonance signals from the patient 15 (but alternatively other RF coils(local coils) can be used for that purpose).

For controlling the basic field magnet 17, the gradient controlprocessor 28 and the radio-frequency antenna control processor 29, themagnetic resonance apparatus 11 has a computer 24. The computer 24centrally controls the magnetic resonance apparatus 11, such as toexecute a predetermined imaging gradient echo sequence. Controlinformation such as imaging parameters, and reconstructed magneticresonance images, can be presented to a user on an output interface 25,such as a display monitor 25, of the magnetic resonance apparatus 11.Furthermore, the magnetic resonance apparatus 11 has an input interface26, via which the user can enter information and/or parameters during ascanning procedure. The computer 24 can include the gradient controlprocessor 28 and/or the radio-frequency antenna control processor 29and/or the output interface 25 and/or the input interface 26.

In the illustrated case the computer 24 it is schematically shown ashaving a first ascertaining processor 33, a second ascertainingprocessor 34 and a correction processor 35. As noted above, although theprocessors 33, 34 and 35 are schematically shown in FIG. 1 as beingwithin the computer 24, any suitable and appropriately connectedcombination of processors can be used and two or more of the processorscan be combined as one processor. The processors may also be consideredas software modules within the computer 24.

The magnetic resonance scanner 13 is operated by the aforementionedcomponents to acquire scan data as well as to acquire a first correctiondata set, a second correction data set, a third correction data set, anda fourth correction data set.

The magnetic resonance apparatus 11 is therefore designed to carry outthe inventive method for magnetic resonance imaging of an examinationobject.

The illustrated magnetic resonance apparatus 11 can of course havefurther components that magnetic resonance apparatuses conventionallyhave. The general manner of operation of a magnetic resonance apparatusis known to those skilled in the art, so a detailed description of thefurther components is not necessary herein.

FIG. 2 is a flowchart of a first embodiment of an inventive method forthe correction of magnetic resonance scan data.

In a first method step CV1 a first correction data set is acquired, byexecution of an echo planar imaging sequence, from a first correctionsub-volume of a correction volume by operation of the MR dataacquisition scanner 13.

In a further method step CV2, a second correction data set is acquired,by execution of the echo planar imaging sequence, from the firstcorrection sub-volume by operation of the MR data acquisition scanner13. The second correction data set is acquired phase shifted in relationto the first correction data set, and the first correction data set andthe second correction data set are acquired one immediately after theother.

In a further method step CI1, a first item of correction information isascertained from the first correction data set and the second correctiondata set with the first ascertaining processor 33.

In a further method step CV3 a third correction data set is acquired, byexecution of the echo planar imaging sequence, from a second correctionsub-volume of the correction volume by operation of the MR dataacquisition scanner 13.

In a further method step CV4, a fourth correction data set is acquired,by execution of the echo planar imaging sequence, from the secondcorrection sub-volume by operation of the MR data set acquisitionscanner 13. The fourth correction data set is acquired phase shifted inrelation to the third correction data set, and the third correction dataset and fourth correction data set are acquired one immediately afterthe other.

In a further method step CI2, a second item of correction information isascertained from the third correction data set and the fourth correctiondata set, with the second ascertaining processor 34.

In a further method step MD, magnetic resonance scan data are acquiredfrom an examination volume by operation of the MR data acquisitionscanner 13.

In a further method step COR, the MR magnetic resonance scan data arecorrected using the first correction information and the secondcorrection information, with the correction processor 35. The magneticresonance scan data corrected in this way, or magnetic resonance imagedata reconstructed from the corrected magnetic resonance scan data, canthen be made available in electronic firm as a data file from thecorrection processor 35. The corrected or reconstructed data can bedisplayed on the output interface 25 and/or be stored in a database.

The following description is essentially limited to the differences fromthe exemplary embodiment in FIG. 2, wherein reference is made withrespect to unchanged method steps to the description of the exemplaryembodiment in FIG. 2. Method steps that are essentially unchanged aredenoted by identical reference numerals.

Embodiments of the inventive method shall be illustrated below in FIG. 3to FIG. 7 according to their sequence over time. FIG. 3 to FIG. 7 canpartially include method steps of the first embodiment of the inventivemethod according to FIG. 2. In addition, the embodiments of theinventive method shown in FIG. 3 to FIG. 7 can comprise additionalmethod steps and sub-steps. A method sequence alternative to FIG. 3 toFIG. 7, which has only some of the additional method steps and/orsub-steps illustrated in FIG. 3 to FIG. 7, is also conceivable. Ofcourse a method sequence alternative to FIG. 3 to FIG. 7 can also haveadditional method steps and/or sub-steps.

FIG. 3 shows a diagram of a sequence over time of a second embodiment ofan inventive method for the correction of magnetic resonance scan data.

FIG. 3 shows that the first correction data set CV1 and the secondcorrection data set CV2 are acquired one immediately after the other.Acquisition of the second correction data set CV2 immediately follows anacquisition of the first correction data set CV1. Of course there canalso be a short break between acquisition of the first correction dataset CV1 and acquisition of the second correction data set CV2, but nofurther scan data are detected during this short break.

There can accordingly be a break between acquisition of the secondcorrection data set CV2 and the third correction data set CV3. Of courseacquisition of the third correction data set CV3 can also immediatelyfollow acquisition of the second correction data set CV2, but this isnot imperative.

According to FIG. 3 the first correction data set CV1, second correctiondata set CV2, third correction data set CV3 and fourth correction dataset CV4 are acquired before acquisition of the magnetic resonance scandata MD. In this way acquisition of the correction data sets CV1, CV2,CV3, CV4 constitutes a pre-scan which is complete as soon as acquisitionof the magnetic resonance scan data MD begins.

In the embodiments of the inventive method shown in FIG. 2 to FIG. 7 thefirst correction data set CV1 and the second correction data set CV2 areacquired from the same first correction sub-volume. The first correctionsub-volume can advantageously constitute a first partial slice stack ofthe correction volume that has, at most, ten first slices of thecorrection volume. The first correction sub-volume most advantageouslyconstitutes a single first slice of the correction volume.

In the embodiments of the inventive method illustrated in FIG. 2 to FIG.7 the third correction data set CV3 and the fourth correction data setCV4 are acquired from the same second correction sub-volume. The secondcorrection sub-volume can advantageously constitute a second partialslice stack of the correction volume that has, at most, ten secondslices of the correction volume. The second correction sub-volume mostadvantageously constitutes a single second slice of the correctionvolume.

FIG. 4 shows a diagram of a sequence over time of a third embodiment ofan inventive method for the correction of magnetic resonance scan data.

In addition to the method sequence illustrated in FIG. 3, FIG. 4 showsthat a first radio-frequency excitation pulse RF1 is used when acquiringthe first correction data set CV1, a second radio-frequency excitationpulse RF2 is used when acquiring the second correction data set CV2, athird radio-frequency excitation pulse RF3 is used when acquiring thethird correction data set CV3 and a fourth radio-frequency excitationpulse RF4 is used when acquiring the fourth correction data set CV4.

The first radio-frequency excitation pulse RF1 and the secondradio-frequency excitation pulse RF2 each excite the spins in the firstcorrection sub-volume. The third radio-frequency excitation pulse RF3and the fourth radio-frequency excitation pulse RF4 each excite thespins in the second correction sub-volume. The radio-frequencyexcitation pulses RF1, RF2, RF3, RF4 each occur at the start ofacquisition of the correction data sets CV1, CV2, CV3, CV4. An EPIreadout train can follow the radio-frequency excitation pulses RF1, RF2,RF3, RF4 in each case for acquisition of the correction data sets CV1,CV2, CV3, CV4.

The first radio-frequency excitation pulse RF1, second radio-frequencyexcitation pulse RF2, third radio-frequency excitation pulse RF3 andfourth radio-frequency excitation pulse RF4 form a radio-frequencyexcitation pulse set, wherein at least one radio-frequency excitationpulse RF1, RF2, RF3, RF4 from a radio-frequency excitation pulse set canhave a flip angle of less than 50°. Furthermore, the firstradio-frequency excitation pulse RF1 and the second radio-frequencyexcitation pulse RF2 can have different first phases from each other.The third radio-frequency excitation pulse RF3 and the fourthradio-frequency excitation pulse RF4 also can have different secondphases from each other.

FIG. 5 shows a diagram of a sequence over time of a fourth embodiment ofan inventive method for the correction of magnetic resonance scan data.

In addition to the method sequence illustrated FIG. 4, FIG. 5 shows thatbetween acquisition of the first correction data set CV1 and of thesecond correction data set CV2 a first spoiler gradient pulse GSP1 isactivated for dephasing a residual magnetism, and between acquisition ofthe third correction data set CV3 and of the fourth correction data setCV4 a second spoiler gradient pulse GSP2 is activated for dephasing aresidual magnetism.

FIG. 6 shows a diagram of a sequence over time of a fifth embodiment ofan inventive method for the correction of magnetic resonance scan data.

According to FIG. 6 acquisition of the magnetic resonance scan data MDcomprises a first scan MD VOL1 of the examination volume, a second scanMD VOL2 of the examination volume and a third scan MD VOL3 of theexamination volume. In this way the examination volume is repeatedlyacquired, in particular in a time series, for example in order toexamine changes over time in the anatomy of the examination object 15.

According to FIG. 6 the first correction data set CV1 and the secondcorrection data set CV2 are acquired between the first scan MD VOL1 andthe second scan MD VOL2 of the examination volume. According to FIG. 6the third correction data set CV3 and the fourth correction data set CV4are acquired between the second scan MD VOL2 and the third scan MD VOL3of the examination volume.

Of course further scans of the examination volume can also take placeduring acquisitions of the magnetic resonance scan data. Cyclicalshifting of the slices acquired in the correction data sets CV1, CV2,CV3, CV4 between the scans MD VOL1, MD VOL2, MD VOL3 of the examinationvolume can take place in particular.

FIG. 7 shows a diagram of a sequence over time of a sixth embodiment ofan inventive method for the correction of magnetic resonance scan data.

As an alternative to the procedure illustrated in FIG. 3 acquisition ofthe magnetic resonance scan data MD should not follow acquisition of thecorrection data sets CV1, CV2, CV3, CV4. Instead, the first correctiondata set CV1, second correction data set CV2, third correction data setCV3 and fourth correction data set CV4 form at least part of themagnetic resonance scan data.

As an example, the first correction data set CV1 and the secondcorrection data set CV2 can be acquired from a first partial slice stackof the examination volume, in particular from a first slice of theexamination volume. The third correction data set CV3 and the fourthcorrection data set CV2 can be acquired from a second partial slicestack of the examination volume, in particular from a second slice ofthe examination volume. Between the second correction data set CV2 andthe third correction data set CV3 additional magnetic resonance scandata VOL PART can optionally be acquired from a third partial slicestack of the examination volume. This procedure can be continued,wherein cyclical shifting of the slices scanned in the correction datasets CV1, CV2, CV3, CV4 occurs.

The method steps of the inventive method illustrated in FIGS. 2 to 7 areimplemented by the computer 24. The computer 24 has the necessarysoftware and/or computer programs for this purpose, which are stored ina memory of the computer 24. The software and/or computer programs haveprogram code (programming instructions) configured to cause theinventive method to be implemented when the code is executed in thecomputer 24.

Although modifications and changes may be suggested by those skilled inthe art, it is the intention of the inventor to embody within the patentwarranted hereon all changes and modifications as reasonably andproperly come within the scope of his contribution to the art.

I claim as my invention:
 1. A method for correcting magnetic resonance(MR) scan data of an examination subject, comprising: operating an MRdata acquisition scanner having a basic magnetic (B0) field therein,while an examination subject is situated therein, to acquire a firstcorrection data set, by executing an echo planar data acquisitionsequence, from a first correction sub-volume of a correction volume ofthe examination subject, said first correction data set having a contentfor use in execution of a correction algorithm that compensates forinhomogeneities in said B0 field; operating the MR data acquisitionscanner, with said B0 field therein, while the examination subject issituated therein, to acquire a second correction data set having acontent for use in execution of said correction algorithm, by executingsaid echo planar data acquisition sequence, from said first correctionsub-volume, with the second correction data set being acquiredphase-shifted with respect to the first correction data set, and withthe first correction data set and the second correction data set beingacquired immediately in succession; providing said first and secondcorrection data sets to a computer and, in said computer, determining afirst item of correction information from said first correction data setand said second correction data set by executing said correctionalgorithm; operating the MR data acquisition scanner, with said B0 fieldtherein, while the examination subject is situated therein, to acquire athird correction data set having a content for use in execution of saidcorrection algorithm, by executing said echo planar data acquisitionsequence, from a second correction sub-volume of said correction volume;operating the MR data acquisition scanner, with said B0 field therein,while the examination subject is situated therein, to acquire a fourthcorrection data set having a content for use in execution of saidcorrection algorithm, by executing said echo planar data acquisitionsequence, from said second correction sub-volume, with the fourthcorrection data set being acquired phase-shifted with respect to thethird correction data set, and with the third correction data set andthe fourth correction data set being acquired in immediate succession;providing said first and second correction data sets to said computerand, in said computer, determining a second item of correctioninformation from said third correction data set and said fourthcorrection data set by again executing said correction algorithm;operating said MR data acquisition scanner, with said B0 field therein,while said examination subject is situated therein, to acquire MR scandata from an examination volume of said examination subject; providingsaid MR scan data to said computer and, in said computer, correctingeffects of said inhomogeneities in said B0 field on said MR scan data byapplying said first item of correction information and said second itemof correction information to said MR scan data, and thereby obtainingcorrected MR scan data; and making the corrected MR scan data availablein electronic form as a data file from said computer.
 2. A method asclaimed in claim 1 wherein said correction volume comprises a pluralityof slices, and operating the MR data acquisition scanner to acquire saidfirst correction sub-volume as a first slice stack of said correctionvolume comprising a number of first slices that is fewer than saidplurality of slices, and operating said MR data acquisition scanner toacquire said second correction sub-volume as a second slice stack ofsaid correction volume comprising a number of second slices that isfewer than said plurality of slices.
 3. A method as claimed in claim 2comprising operating said MR data acquisition scanner to acquire saidfirst correction sub-volume as, at most, ten first slices of saidcorrection volume, and to acquire said second correction sub-volume as,at most, ten second slices of said correction volume.
 4. A method asclaimed in claim 2 comprising operating said MR data acquisition scannerto acquire said first correction sub-volume as a single first slice ofsaid correction volume, and to acquire said second correction sub-volumeas a single second slice of said correction volume.
 5. A method asclaimed in claim 1 comprising: operating said MR data acquisitionscanner to acquire said first correction data set by radiating a firstradio-frequency excitation pulse when executing said echo planar dataacquisition sequence; operating said MR data acquisition scanner toacquire said second correction data set by radiating a secondradio-frequency excitation pulse when executing said echo planar dataacquisition sequence; operating said MR data acquisition scanner toacquire said third correction data set by radiating a thirdradio-frequency excitation pulse when executing said echo planar dataacquisition sequence; and operating said MR data acquisition scanner toacquire said fourth correction data set by radiating a fourthradio-frequency excitation pulse when executing said echo planar dataacquisition sequence.
 6. A method as claimed in claim 5 comprisingoperating said MR data acquisition scanner to radiate at least one ofsaid first radio-frequency excitation pulse, said second radio-frequencyexcitation pulse, said third radio-frequency excitation pulse, and saidfourth radio-frequency excitation pulse, with a flip angle of less than50°.
 7. A method as claimed in claim 5 comprising operating said MR dataacquisition scanner to radiate said first radio-frequency excitationpulse and the second radio-frequency excitation pulse with respectivelydifferent first phases from each other, and to radiated said thirdradio-frequency excitation pulse and said fourth radio-frequencyexcitation pulse with respectively different second phases from eachother.
 8. A method as claimed in claim 1 comprising operating said MRdata acquisition scanner to activate a first spoiler gradient betweenacquiring said first correction dataset and said second correction dataset, which dephases residual magnetism of nuclear spins in saidcorrection volume that exists after acquiring said first correction dataset, and operating said MR data acquisition scanner to activate a secondspoiler gradient between acquiring said third correction data set andsaid fourth correction data set, which dephases residual magnetism thatexists in said correction volume after acquiring said third correctiondata set.
 9. A method as claimed in claim 1 comprising operating said MRdata acquisition scanner to acquire each of said first correction dataset, said second correction data set, said third correction data set,and said fourth correction data set before acquiring said MR scan data.10. A method as claimed in claim 1 comprising operating said MR dataacquisition scanner to acquire said MR scan data in a first scan of theexamination volume, a second scan of the examination volume, and a thirdscan of the examination volume and to acquire first correction data setand said second correction data set between said first scan and saidsecond scan, and to acquire said third correction data set and saidfourth correction data set between said second scan and said third scan.11. A method as claimed in claim 1 comprising operating said MR dataacquisition scanner to acquire said first correction data set, saidsecond correction data set, said third correction data set and saidfourth correction data set as at least a portion of said MR scan data.12. A magnetic resonance (MR) apparatus, comprising: an MR dataacquisition scanner; a computer configured to operate said MR dataacquisition scanner having a basic magnetic (B0) field therein, while anexamination subject is situated therein, in the scanner to acquire afirst correction data set, by executing an echo planar data acquisitionsequence, from a first correction sub-volume of a correction volume ofthe examination subject, said first correction data set having a contentfor use in execution of a correction algorithm that compensates forinhomogeneities in said B0 field; said computer being configured tooperate the MR data acquisition scanner, with said B0 field therein,while the examination subject is situated therein, to acquire a secondcorrection data set having a content for use in execution of saidcorrection algorithm, by executing said echo planar data acquisitionsequence, from said first correction sub-volume, with the secondcorrection data set being acquired phase-shifted with respect to thefirst correction data set, and with the first correction data set andthe second correction data set being acquired immediately in succession;said computer being configured to determine a first item of correctioninformation from said first correction data set and said secondcorrection data set by executing said correction algorithm; saidcomputer being configured to operate the MR data acquisition scanner,with said B0 field therein, while the examination subject is situatedtherein, to acquire a third correction data set having a content for usein execution of said correction algorithm, by executing said echo planardata acquisition sequence, from a second correction sub-volume of saidcorrection volume; said computer being configured to operate the MR dataacquisition scanner, with said B0 field therein, while the examinationsubject is situated therein, to acquire a fourth correction data sethaving a content for use in execution of said correction algorithm, byexecuting said echo planar data acquisition sequence, from said secondcorrection sub-volume, with the fourth correction data set beingacquired phase-shifted with respect to the third correction data set,and with the third correction data set and the fourth correction dataset being acquired in immediate succession; said computer beingconfigured to determine a second item of correction information fromsaid third correction data set and said fourth correction data set byagain executing said correction algorithm; said computer beingconfigured to operate said MR data acquisition scanner, with said B0field therein, while said examination subject is situated therein, toacquire MR scan data from an examination volume of said examinationsubject; said computer being configured to correct effects of saidinhomogeneities in said B0 field on said MR scan data by applying saidfirst item of correction information and said second item of correctioninformation to said MR scan data, and thereby obtaining corrected MRscan data; and said computer being configured to make the corrected MRscan data available in electronic form as a data file from saidcomputer.
 13. A non-transitory, computer-readable data storage mediumencoded with programming instructions, said storage medium being loadedinto a computer of a magnetic resonance (MR) apparatus that comprises anMR data acquisition scanner having a basic magnetic (B0) field therein,said programming instructions causing said computer to: operate said MRdata acquisition scanner, while an examination subject is situatedtherein, to acquire a first correction data set, by executing an echoplanar data acquisition sequence, from a first correction sub-volume ofa correction volume of the examination subject, said first correctiondata set having a content for use in execution of a correction algorithmthat compensates for inhomogeneities in said B0 field; operate the MRdata acquisition scanner, with said B0 field therein, while theexamination subject is situated therein, to acquire a second correctiondata set having a content for use in execution of said correctionalgorithm, by executing said echo planar data acquisition sequence, fromsaid first correction sub-volume, with the second correction data setbeing acquired phase-shifted with respect to the first correction dataset, and with the first correction data set and the second correctiondata set being acquired immediately in succession; determine a firstitem of correction information from said first correction data set andsaid second correction data set by executing said correction algorithm;operate the MR data acquisition scanner, with said B0 field therein,while the examination subject is situated therein, to acquire a thirdcorrection data set having a content for use in execution of saidcorrection algorithm, by executing said echo planar data acquisitionsequence, from a second correction sub-volume of said correction volume;operate the MR data acquisition scanner, with said B0 field therein,while the examination subject is situated therein, to acquire a fourthcorrection data set having a content for use in execution of saidcorrection algorithm, by executing said echo planar data acquisitionsequence, from said second correction sub-volume, with the fourthcorrection data set being acquired phase-shifted with respect to thethird correction data set, and with the third correction data set andthe fourth correction data set being acquired in immediate succession;determine a second item of correction information from said thirdcorrection data set and said fourth correction data set by againexecuting said correction algorithm; operate said MR data acquisitionscanner, with said B0 field therein, while said examination subject issituated therein, to acquire MR scan data from an examination volume ofsaid examination subject; correct effects of said inhomogeneities insaid B0 field on said MR scan data by applying said first item ofcorrection information and said second item of correction information tosaid MR scan data, and thereby obtaining corrected MR scan data; andmake the corrected MR scan data available in electronic form as a datafile from said computer.
 14. A non-transitory, computer-readable datastorage medium as claimed in claim 13, wherein said correction algorithmis used in combination with the Phase Labeling For Additional CoordinateEncoding (PLACE) algorithm.
 15. A method as claimed in claim 1, whereinsaid correction algorithm is used in combination with the Phase LabelingFor Additional Coordinate Encoding (PLACE) algorithm.
 16. An MRapparatus as claimed in claim 12, wherein said correction algorithm isused in combination with the Phase Labeling For Additional CoordinateEncoding (PLACE) algorithm.